fiber optical sensors in cms s. buontempo on behalf of the fos4hep group cms tracker monitoring...

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Fiber Optical Sensors in CMS S. Buontempo on behalf of the FOS4HEP Group CMS Tracker Monitoring meeting, April 6 th 2011

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Fiber Optical Sensors in CMS

S. Buontempoon behalf of the FOS4HEP Group

CMS Tracker Monitoring meeting, April 6th 2011

Outlook

2

Salvatore (5 min)• FOS technique: Fiber Bragg Grating• FOS in CMS

Zoltan/Noemi (20 min)• 1y FOS measurements in 2010• Bulkhead FOS vs Tracker T (Maki)• Additional UXC T measurements in 2011• FOS data in S4CMS project

Salvatore/Paolo (20 min)• Preliminary R&D results on new FOS

applications• FOS4HEP project

FOS Technique

3

effB n2

Where:neff is the effective refractive index of the fiber,

Λ is the grating pitch and

λB is the reflected Bragg wavelength.

TEMPERATURE CHANGE

Thermal expansion for Termo-optic effect for

STRESS

Elasto-optic effect forDirect Strain for

effn

effn

FOS Technique

4

Temperature Sensitivity ≈10pm/°K

@ λB=1550nm

T

STRAIN AND TEMPERATURE Sensitivity : FBG Spectral Response (Temperature)

FBG SPECTRAL RESPONSE: Temperature Shift

FOS Technique

5

STRAIN AND TEMPERATURE Sensitivity: FBG Spectral Response (Axial Strain)

FBG SPECTRAL RESPONSE: Axial Strain Shift

Strain Sensitivity ≈1pm/με

@ λB=1550nm

ε

For more details: see Prof. Breglio and Prof. Giordano technical seminar in CMShttps://indico.cern.ch/conferenceDisplay.py?confId=56088

FOS Sensors in CMS

• Sensors placed to the following regions in CMS:– HF region negative side (Raiser and Castor table 10-6)– Tracker bulkhead on both side (10-10 sensor)– Experimental Cavern (60) in January 2011

6

in july 2009

Aim:

• demonstrate feasibility• monitor mechanical

deformation induced by B field (HF-/Castor)

• monitor T in tracker bulkhead• (2011) monitor T gradient in

UXC

Position of BulkHead Temperature sensors

7

Positive side:

Position of BulkHead Temperature sensors

8

Negative side:

Position of CASTOR Platform sensors

9

Position of sensors on the Raiser

10

ZOLTAN TALK

11

• 1y FOS measurements in 2010• Bulkhead FOS vs Tracker T (Maki)• Additional UXC T measurements in 2011

• FOS data in S4CMS project

PRELIMINARY R&D RESULTS ON NEW FOS APPLICATIONS

2011.03.03. 12FOS operation in CMS

13

Preliminary results on new FOS

In 2010 3 lines of R&D activities on FOS techniques have started for HEP applications:

• Low and precise RH in negative T environment (P. Petagna)

• B field (A. Gaddi)

• T and strain in cryogenic conditions (M. Bajko)

Cladding Core

Bragg Grating

Buffer

FBG sensor

Coating Material

By using a functionalized coating material,i.e. mechanically sensible to:B field or Humidity or “Cryo T”

Status of R&D on RH FOS @ PH/DTPaolo Petagna (CERN PH/DT)

•Motivations

•PH/DT test set-up

•Phase I: tip-coated (NFFP) oxide sensors

•Phase II: FBG polyimide sensors

•Phase III: new collaboration agreement

• Almost all miniaturized humidity sensors presently available on the market are electronic sensors (mainly capacitive-based, followed by resistive-based).

• Despite all efforts, these sensors still fail to provide a complete set of favourable characteristics, e.g., good linearity, high sensitivity, low uncertainty, low hysteresis and rapid response time.

• For an application in HEP detectors, one should add to this the sensitivity to electro-magnetic noise pick-up, the suitability for multi-point distributed measurements and the resistance to ionizing radiations.

Motivations

Nowadays – although important requirements on environmental control exist, in particular for Trackers –

there is no miniaturized humidity sensor on the market well suited for HEP detector applications

Paolo Petagna (CERN PH/DT)

PH/DT test set-up

Test section

Thermally controlled liner

Salt solution container (if needed)

External air circulation(dry + saturated air mixer)

Closed loop circulation(salt solution in box)

Chilled mirror

Ranges:0% ≤ RH ≤ 100%

-20 °C ≤ T ≤ +30 °C

Insulated confinement

Paolo Petagna (CERN PH/DT)

Phase I: tip-coated (NFFP) oxide sensors

X axis: 10 µm

Y axis: 10 µm

Fiel

dIn

tens

ity(A

.U.)

X axis: 10 µm Y axis: 10 µm

Surf

ace

peak

she

ight

(µm

)

Optimal SnO2 deposition: sub-wavelength bumps spaced by sub-wavelength distances (wavelength = 1.55 mm)

Build on previous experience of partner institutes (Unisannio, CNR-IMCB, DIBET) on Near-Field Fabry-Perot sensors for chemical applications

Paolo Petagna (CERN PH/DT)

Phase I: tip-coated (NFFP) oxide sensors

• Very good results obtained with two sensors on steady and dynamical behaviour between +20 °C and -20 °C

• Paper submitted to Sensors and Actuators• Patent application filed

BUT EXTREMELY DIFFICULT TO REPRODUCE THE GOOD CONFIGURATION

Paolo Petagna (CERN PH/DT)

Phase I: tip-coated (NFFP) oxide sensors

Help sought in PH/DT (A. Braem / T. Schneider) and TE/VSC (M.Taborelli) to investigate possible way to stabilize the production and obtain a reasonable yield

Two possible techniques have been envisaged and will be tried. Work performed on a “courtesy” base (i.e. depending on available windows), time scale not clear at the moment

Paolo Petagna (CERN PH/DT)

Phase II: FBG + polyimide sensors

Two examples have been recently reported in literature about successful use of polyimide-coated FBG as relative humidity sensors: Kronemberg et al: Relative humidity sensor with optical fiber Bragg gratings, Optics Letters Vol. 27, No. 16 (2002)Yeo et al: Characterisation of a polymer-coated fibre Bragg grating sensor for relative humidity sensing. Sensors and Actuators B, 110 (2005)

Extremely interesting results between +20 C and – 20 C are being obtained in CERN PH/DT test set-up on two commercial FBG polyimide-coated in a non controlled way by the producer (insulation coating)

-20 0 20 40 60 80 100 1204,5

4,6

4,7

4,8

4,9

5,0

5,1

5,2

5,3

5,4

Vn

T1

RH DPM(%)

prova del 24-25-26 gennaio T=20° prova del 27 gennaio e 1-2 febbraio a T=0°C prova del 31 gennaio e 1-2 febbraio a T=0°C prova del 7-8 febbraio a T= -15°C

-20 0 20 40 60 80 100 1204,0

4,2

4,4

4,6

4,8

5,0

prova del 24-25-26 gennaio T=20° prova del 27 gennaio e 1-2 febbraio a T=0°C prova del 31 gennaio e 1-2 febbraio a T=0°C prova del 7-8 febbraio a T= -15°C

Vn

FB

G2

RH DPM(%)

Paolo Petagna (CERN PH/DT)

• Similar sensors can be rather easily produced under controlled conditions by dip coating or by mould coating in a standard UV recoater

• Launched programme to investigate:radiation hardness, effect of coating thickness, effect of polyimide type, reproducibility of the sensor, stability in time

• 10 commercial sensors (few mm polyimide coating) ordered (CMS tracker funds) from an external commercial producer (that can secure at least always the same type of polymide coating). Received at CERN last week. Measurements will start in next days.

• 10 custom sensors ordered (CMS tracker funds) and being produced in different (controlled) thicknesses @ CNR-IMCB. Delivery

• Test production launched in parallel @ CERN (collaboration with TE/MPA)

Phase II: FBG + polyimide sensors

Paolo Petagna (CERN PH/DT)

Phase III: new collaboration agreement

Collaboration agreement for 2011 defined, now under signature process

Programme:LPG multi sensors coated with different oxydes (Sol-Gel deposition) Partners: Unisannio + Uninapoli Federico II (DIBET)

FBG multi sensors coated with fully cured epoxy Partners: CNR Napoli (IMCB) + Uninapoli Federico II (DIBET)

Results expected: Dec 2011

Paolo Petagna (CERN PH/DT)

FOS for B field measurements

Magnetostrictivematerial

FBGHolder

The FBG sensor is glued onto a Magnetostrictive material which changes its shape in function of applied magnetic field. All is placed in a proper holder which produces an initial controlled pre-stress condition.

5 sensors tested

Goal: measure B field at low and high ranges (A. Gaddi)

Preliminary results: Good reproducibility, good linearity in range 500-3500G, small hysteresis and impressive sensitivity (2mV/G)

FOS operation in CMS 27

FOS for Cryo T and strainmeasurements

Goal: measure T and strain in cryogenic conditions (M. Bajko)

The FBG sensor is glued onto a thermostrictive material shrinking up to cryogenic temperatures. Test measurements done @77K and @1.9K

Preliminary results show good reliability and sensitivity up to 1.9K with a single sensor type. Patent option being evaluated.

FOS4HEP project

• idea is to get funding to increase the strengh of the FOS activities at CERN and in involved group sites• First proposal submitted to EU-PEOPLE-MC call in dec 2009. Final score was 76/100, over the threshold of 70/100, but not selected for negotiation phase.• Second proposal edited with help of PNO external consultancy and submitted in EU-PEOPLE-MC call in jan 2011. Result expected by May 2011.

FOS4HEP Participants

3 additional associated partners (Ansaldo SC, Babcock Noell, AMS techn.) not included due to late letter of commitment

FOS4HEP architecture

FOS4HEP Fellows

14 PhD (3years) and 3 post-Doc (2Years) fellows requested

Summary

2011.03.03. FOS operation in CMS 32

• During 2009 & 2011 ~100 FBG sensors have been installed in CMS

• An automatic DAQ of FBGs has been set up

• FOS system is in 24/7 operation since a year and could follow:- Tracker operation (temperature)- Magnet cyles induced mechanical changes of HF-

• Recently additional 60 T-sensing FOS network has been installed in UXC, monitoring T gradient

• FOS data are integrated into the Sensors4CMS project

• 3 R&D projects were started on the FOS technology for RH, Bfield and Cryogenic applications. Preliminary results look very promising

• FOS4HEP community created and a funding request submitted to EU call.